📝 SummarXiv

Abstract

The recently reported gate-tunable superconductivity in monolayer WTe$_2$ exhibits several striking anomalies beyond the standard paradigm, including a contrasting carrier-density dependence of the transition temperature $T_c$ in weakly and strongly disordered regimes and more surprisingly, the sudden disappearance of superconducting fluctuations below a critical carrier density. To understand these features, we go beyond the mean-field theory to treat the superconducting gap and superfluid density by explicitly incorporating both Nambu-Goldstone (NG) phase fluctuations and Berezinskii-Kosterlitz-Thouless (BKT) fluctuations. We show that these fluctuations are minimal in the weak-disorder regime but become crucial under strong disorder, where the zero-temperature gap renormalized by NG quantum fluctuations becomes density-dependent while the BKT fluctuations drive the superconducting $T_c$ below the gap-closing temperature. Simulations within this unified framework combining with the density-functional-theory input to account for the excitonic instability quantitatively reproduced nearly all key experimental observations in monolayer WTe$_2$, providing a consistent understanding of reported anomalies.